Deep Mixing of 3 He: Reconciling Big Bang and Stellar Nucleosynthesis

Author:

Eggleton Peter P.123,Dearborn David S. P.123,Lattanzio John C.123

Affiliation:

1. Institute of Geophysics and Planetary Physics, Lawrence Livermore National Laboratory, 7000 East Avenue, Livermore, CA 94551, USA.

2. Physics and Applied Technologies Division, Lawrence Livermore National Laboratory, 7000 East Avenue, Livermore, CA 94551, USA.

3. Centre for Stellar and Planetary Astrophysics, Monash University, Australia.

Abstract

Low-mass stars, ∼1 to 2 solar masses, near the Main Sequence are efficient at producing the helium isotope 3 He, which they mix into the convective envelope on the giant branch and should distribute into the Galaxy by way of envelope loss. This process is so efficient that it is difficult to reconcile the low observed cosmic abundance of 3 He with the predictions of both stellar and Big Bang nucleosynthesis. Here we find, by modeling a red giant with a fully three-dimensional hydrodynamic code and a full nucleosynthetic network, that mixing arises in the supposedly stable and radiative zone between the hydrogen-burning shell and the base of the convective envelope. This mixing is due to Rayleigh-Taylor instability within a zone just above the hydrogen-burning shell, where a nuclear reaction lowers the mean molecular weight slightly. Thus, we are able to remove the threat that 3 He production in low-mass stars poses to the Big Bang nucleosynthesis of 3 He.

Publisher

American Association for the Advancement of Science (AAAS)

Subject

Multidisciplinary

Reference23 articles.

1. Stellar Evolution.VI. Evolution from the Main Sequence to the Red-Giant Branch for Stars of Mass 1 M_{sun}, 1.25 M_{sun}, and 1.5 M_{sun}

2. The initial value for 3 He that we assumed is somewhat higher than the mass-fraction (∼5 × 10 –5 ) implied by ( 19 ). This is partly because we assume that primordial deuterium of comparable abundance is wholly burnt into 3 He before the computation starts. However the important point is that the great bulk of the 3 He in the RG phase is what was synthesized from ordinary hydrogen during the MS phase not what was there initially. The enrichment factor of 8 that we mention above would be a factor of ∼16 if we started with half as much 3 He but the abundance level of ∼1.6 × 10 –3 would be very much the same.

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